Drell-Yan Di-Lepton Production Why Drell-Yan? Asymmetries depend on PD only (SIDIS→convolution with QFF) Why ? Each valence quark can contribuite to the.

Slides:

Advertisements

Similar presentations

1 First Measurement of the Structure Function b 1 on Tensor Polarized Deuteron Target at HERMES A.Nagaitsev Joint Institute for Nuclear Research, Dubna.

Advertisements

Exploring the Structure of the Pion Paul E. Reimer Physics Division Argonne National Laboratory 14 October Why are we interested in the pion? 2.What.

W/Z Production at the LHC and the Parton Distributions C.S. Kim (w/ Y.S. Jeong, F. Halzen)

1 Partonic Substructure of Nucleons and Nuclei with Dimuon Production Partonic structures of the nucleons and nuclei with dimuon production –Overview and.

Delia Hasch TMDs & friends from lepton scattering -experimental overview- INT workshop on “3D parton structure of the nucleon encoded in GPDs & TMDs”,

 Transverse Polarization in STAR Au-Au Collisions Polarization definition and models E896 results STAR analysis STAR results Significance of results Future.

Working Group on e-p Physics A. Bruell, E. Sichtermann, W. Vogelsang, C. Weiss Antje Bruell, JLab EIC meeting, Hampton, May Goals of this parallel.

V. Abazov 1, G. Alexeev 1, M. Alexeev 2, A. Amoroso 2, N. Angelov 1, M. Anselmino 3, S. Baginyan 1, F. Balestra 2, V. A. Baranov 1, Yu. Batusov 1, I. Belolaptikov.

Simulations of Single-Spin Asymmetries from EIC Xin Qian Kellogg, Caltech EIC Meeting at CUA, July 29-31, TMD in SIDIS 2.Simulation of SIDIS.

1 Updates on Transversity Experiments and Interpretations Jen-Chieh Peng Transversity Collaboration Meeting, JLab, March 4, 2005 University of Illinois.

THE DEEP INELASTIC SCATTERING ON THE POLARIZED NUCLEONS AT EIC E.S.Timoshin, S.I.Timoshin.

Drell-Yan Perspectives at FAIR Marco Destefanis Università degli Studi di Torino Drell-Yan Scattering and the Structure of Hadrons Trento (Italy) May 21-25,

T.C. Jude D.I. Glazier, D.P. Watts The University of Edinburgh Strangeness Photoproduction: Polarisation Transfer & Cross-Section Measurements.

Polarisation transfer in hyperon photoproduction near threshold Tom Jude D I Glazier, D P Watts The University of Edinburgh.

T.C. Jude D.I. Glazier, D.P. Watts The University of Edinburgh Strangeness Photoproduction At Threshold Energies.

Highlights from the COMPASS experiment QNP09, Beijing, September 2009 G. K. Mallot CERN/PH for the Collaboration.

1 Flavor Symmetry of Parton Distributions and Fragmentation Functions Jen-Chieh Peng Workshop on “Future Prospects in QCD at High Energy” BNL, July 17-22,

Possibilities to perform DVCS measurement at COMPASS E. Burtin CEA-Saclay Irfu/SPhN On Behalf of the COMPASS Collaboration DIS Madrid - 29 April,

International Workshop on Transverse Polarisation Phenomena in Hard Processes Como, September 7- 10, 2005 Marco Maggiora Dipartimento di Fisica ``A. Avogadro''

Detector requirement form TMD working group J. P. Chen for the TMD working group June 5, 2010, EIC Detector Workshop, JLab TMD Program - A lot of enthusiasm,

Study of the to Dilepton Channel with the Total Transverse Energy Kinematic Variable Athens, April 17 th 2003 Victoria Giakoumopoulou University of Athens,

Single-spin asymmetries in two hadron production of polarized deep inelastic scattering at HERMES Tomohiro Kobayashi Tokyo Institute of Technology for.

Future Physics at JLab Andrew Puckett LANL medium energy physics internal review 12/14/

May 17, 2006Sebastian Baunack, PAVI06 The Parity Violation A4 Experiment at forward and backward angles Strange Form Factors The Mainz A4 Experiment Result.

MENU2004, Bejing, August 29- September 5, 2004 Raimondo Bertini Dipartimento di Fisica ``A. Avogadro'' and INFN - Torino, Italy Λ POLARISATION TO PROBE.

Improved Measurement of d/u Asymmetry in the Nucleon Sea

Measuring the charged pion polarizability in the  →    −  reaction David Lawrence, JLab Rory Miskimen, UMass, Amherst Elton Smith, JLab.

1 Possible Additional Measurements in E906 Azimuthal angular distributions of Drell-Yan and J/ Ψ p+d/p+p ratios for J/ Ψ production Nuclear effects of.

Kaon Production on the Nucleon D. G. Ireland MENU Rome, September 30 – October 4, 2013.

R. Joosten, Oct. 7, 2008 Measurement of TMDs in Semi-Inclusive DIS in Semi-Inclusive DIS Rainer Joosten University of Bonn Charlottesville, VA, October.

Oct 6, 2008Amaresh Datta (UMass) 1 Double-Longitudinal Spin Asymmetry in Non-identified Charged Hadron Production at pp Collision at √s = 62.4 GeV at Amaresh.

Liu Minghui Nanjing MC study of W polarization and ttbar spin correlation Liu Minghui, Zhu Chengguang April 27, 2008.

1 Probing Spin and Flavor Structures of the Nucleon with Hadron Beams Flavor and spin structures of the nucleons –Overview and recent results Future prospects.

I R F U DRELL-YAN at COMPASS Stephane Platchkov I nstitut de R echerche sur les lois F ondamentales de l’ U nivers CEA/IRFU, Saclay, France GDR Nucléon.

Physics to be explored by the un-polarized Drell-Yan program in COMPASS experiment Wen-Chen Chang Institute of Physics, Academia Sinica, Taiwan on behalf.

1 Azimuthal dependence in unpolarized proton-induced Drell-Yan processes Mini-symposium on orbital motion of quarks in hard scattering 2 nd joint meeting.

Drell-Yan pairs from pion scattering on longitudinally polarized nucleons COMPASS DY meeting, Torino, March Oleg Teryaev BLTP, JINR, Dubna.

Marco Maggiora Dip. “A. Avogadro” – Università e INFN - Torino Commissione I — Roma, Maggio 2004 ASSIA LOI Dzhelepov Laboratory of Nuclear Problems,

HERMES results on azimuthal modulations in the spin-independent SIDIS cross section Francesca Giordano DESY, Hamburg For the collaboration Madrid, DIS.

Possibility of direct extraction of the transversitiy from polarized Drell-Yan measurement in COMPASS Transversity Drell-Yan for transverstiy transverse.

1 Quarkonium Production at J-PARC Quarkonium Production at J-PARC with Unpolarized Proton Beam Quarkonium Production at J-PARC with Polarized Beam and.

Latest results from COMPASS TMD physics Anna Martin Trieste University & INFN on behalf of the COMPASS Collaboration.

High-energy hadron physics at J-PARC Wen-Chen Chang 章文箴 Institute of Physics, Academia Sinica, Taiwan KEK theory center workshop on Hadron physics with.

Polarised DIS Experiment Gerhard Mallot. G. Mallot/CERN Spin Summer School, BNL, 2004 Plan Lecture I –introduction –kinematics –the cross section –structure.

Polarisation transfer in hyperon photoproduction near threshold Tom Jude D I Glazier, D P Watts The University of Edinburgh.

 0 life time analysis updates, preliminary results from Primex experiment 08/13/2007 I.Larin, Hall-B meeting.

Fragmentation of relativistic 9 Be and 14 N nuclei in nuclear track emulsion D. A. Artemenkov JINR, Dubna BECQUREL Collaboration web site:

Azimuthal Asymmetry In The Unpolarized Drell-Yan Process Zhou Jian ShanDong University, China & LBNL, US Collaborators: Feng Yuan (LBNL, US) Zuo-tang Liang.

R. Joosten, Oct. 7, 2008 Measurement of TMDs in Semi-Inclusive DIS in Semi-Inclusive DIS Rainer Joosten University of Bonn Charlottesville, VA, October.

The PAX Project and HEPI TSU Contribution 06 August, GGSWBS’12, Tbilisi. Mirian Tabidze High Energy Physic Institute of TSU.

Spin Physics at RHIC Ming Xiong Liu Los Alamos National Lab 8/3/091Ming Xiong Liu OCPA06.

Exclusive Vector Meson Electroproduction at 12 GeV Paul Stoler Rensselaer Polytechnic Institute.

1 DIS 2007, Munich, April 19, 2007 Aram Kotzinian Beyond Collins and Sivers: further measurements of the target transverse spin-dependent azimuthal asymmetries.

Drell-Yan Studies in ppbar Reactions at FAIR Marco Destefanis Università degli Studi di Torino 43 rd PANDA Collaboration Meeting GSI, Darmstadt (Germany)

Feasibility studies for DVCS and first results on exclusive  at COMPASS DVCS studies Physics impact Experimental issues Recoil detector prototype Exclusive.

Quarkonia production with the HERA-B experiment J. Spengler, MPI Heidelberg.

Future Drell-Yan program of the COMPASS cllaboration Norihiro DOSHITA (Yamagata University) On behalf of the COMPASS collaboration 2016/7/31N. Doshita.

Round table discussion

Unpolarized Azimuthal Asymmetries from the COMPASS Experiment

Plans for nucleon structure studies at PANDA

Transverse parton distribution functions

New Results for Transverse Spin Effects at COMPASS

past and future experiments

past and future experiments

Quark and Gluon Sivers Functions

Single Spin Asymmetry with a Transversely Polarized

J. Rak (for R. Hobbs) For the PHENIX collaboration

Greg Heath University of Bristol

Spin Studies via Drell-Yan Process at PANDA

Angular Distribution in Unpolarized Proton-induced Drell-Yan Process

Presentation transcript:

Drell-Yan Di-Lepton Production Why Drell-Yan? Asymmetries depend on PD only (SIDIS→convolution with QFF) Why ? Each valence quark can contribuite to the diagram Kinematics x F =x 1 -x 2 x1x2x1x2

Drell-Yan Di-Lepton Production Scaling: Full x 1,x 2 range. needed [1] Anassontzis et al., Phys. Rew. D38 (1988) 1377

Drell-Yan Asymmetries Polarised beam and target To be corrected for: NH 3 polarised target:

Drell-Yan Asymmetries Unpolarised beam and target Di-Lepton Rest Frame NLO pQCD: λ  1,   0,  0 Experimental data [1] :  30 % [1] J.S.Conway et al., Phys. Rev. D39(1989)92. involves transverse spin effects at leading twist [2] : cos2φ contribution to angular distribution provide: [2] D. Boer et al., Phys. Rev. D60(1999)

Angular distribution in CM frame  - + N   + +  GeV/c -0.6 < cos < < M < 8.5 GeV/c 2 cut on P T selects asymmetry 30% asymmetry observed Conway et al, Phys. Rew. D39 (1989) 92

Drell-Yan Asymmetries Unpolarised beam, polarised target Even unpolarised beam is a powerful tool to investigate к T dependence of QDF D. Boer et al., Phys. Rev. D60(1999)

Weak decay B.R. = 0.9 % events / 100 days [1] Smith and Vogt Z. Phys. C75 (1997)271